Abstract

Motivated by the recent findings that the ratio $\varepsilon'/\varepsilon$ in the Standard Model (SM) appears to be significantly below the data we investigate whether the necessary enhancement of this ratio can be obtained in 331 models, in which new physics (NP) contributions to $\varepsilon'/\varepsilon$ and other flavour observables are dominated by tree-level exchanges of a $Z^\prime$. NP contributions to $\varepsilon'/\varepsilon$ in these models are governed by the electroweak operator $Q_8$ for which the hadronic matrix element is rather well known so that our analysis of NP contributions is subject to much smaller uncertainties than within the SM. We consider seven 331 models selected in our earlier analysis on the basis of electroweak precision data. Imposing the constraints from $\Delta F=2$ transitions we find that only three of these models can provide a significant positive shift in $\varepsilon'/\varepsilon$ up to $6\times 10^{-4}$ for $M_{Z^\prime}=3$ TeV. Two of them allow simultaneously a supression of ${\cal B}(B_{s}\to \mu^+\mu^-)$ by $20\%$, bringing the theory closer to the data without any significant impact on the Wilson coefficient $C_9$. The third one provides also the shift $\Delta C_9=-0.6$, softening the anomalies in $B\to K^*\mu^+\mu^-$, without any significant impact on $B_{s}\to \mu^+\mu^-$. NP effects in rare $K$ decays and in $B\to K(K^*)\nu\bar\nu$ turn out to be small. The flavour structure of 331 models implies that even for $M_{Z^\prime}=30$ Tev a shift of $\varepsilon'/\varepsilon$ up to $8\times 10^{-4}$ and a significant shift in $\varepsilon_K$ can be obtained, while the effects in other flavour observables are small.

Highlights

  • Recent analyses addressing the implications of new value of ε /ε within the Standard Model (SM) for new physics (NP) in the Littlest Higgs model with T-parity and simplified Z and Z models can be found in [5] and [6], respectively

  • In these models new physics (NP) contributions to ε /ε and other flavour observables are dominated by tree-level exchanges of a Z with non-negligible contributions from tree-level Z exchanges generated through the Z −Z mixing

  • Considering first seven 331 models selected by us in [4] by electroweak precision tests and requiring a shift ∆(ε /ε) ≥ 4.0 × 10−4 by NP, we reduced the number of 331 models to three: M8, M9 and M16 in the terminology of [4]

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Summary

Preliminaries

In 331 models ε /ε receives the dominant new contribution from tree-level Z exchanges but through Z − Z mixing, analyzed in detail in [4], contributions from tree-level Z exchanges in certain models and for certain values of new parameters cannot be neglected. We begin with general expressions valid for both Z and Z contributions which will allow us to recall all the relevant parameters of the 331 models. We will specify these expressions to Z and Z cases which differ only by the value of the Wilson coefficient of the Q8 operator at the low renormalization scale at which the relevant hadronic matrix element of Q8 is calculated. In evaluating (2.1) we use, as in the case of the SM, the experimental values for ReA2 and εK : ReA2 = 1.210(2) × 10−8 GeV, |εK | = 2.228(11) × 10−3. The value of ReA2 in (2.2) is by this factor smaller than in [1]. F2 corresponds to the case in which the choice of triplets and antitriplets is reversed.

Z contribution
Favourite 331 models
Z outside the reach of the LHC
TeV MZ
Summary
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